Analyzing the Function f(t)
The function is defined as f(t)=t2∣t+1∣. Because the modulus sign creates a point of non-differentiability at t=−1, we must analyze the function in two distinct regimes: t<−1 and −1≤t<0.
For the region t<−1, the expression t+1 is negative, which forces the modulus to reveal itself as −(t+1). This transforms our function into:
Finding the Monotonicity
Applying the quotient rule to f(t)=t2−t−1, we calculate the derivative:
f′(t)=(t2)2(−1)(t2)−(−t−1)(2t)=t4−t2+2t2+2t=t4t2+2t=t3t+2
In the territory where t<−1, the denominator t3 is always negative. For the function to be strictly decreasing, we require f′(t)<0, which implies the numerator t+2 must be positive.
This leads us to the interval (−2,−1). Comparing this to the given interval (2α,α), we deduce that 2α=−2 and α=−1. Thus, we find α=−1.
Analyzing the Function g(x)
With α secured, we examine the function g(x)=2ln(x−2)−x2+4x+1. This function is defined for x>2, which serves as our strict boundary.
To find the local maximum, we seek the critical points where the slope of the tangent, g′(x), is zero:
Setting g′(x)=0 leads to the following algebraic manipulation:
x−22=2x−4
x−22=2(x−2)
(x−2)2=1
Final Calculation and Verification
Solving (x−2)2=1 yields x−2=1 or x−2=−1, resulting in x=3 or x=1. Given our boundary constraint x>2, we discard x=1 and accept x=3.
To confirm this is a local maximum, we use the second derivative test:
At x=3, we find g′′(3)=−12−2=−4. Since g′′(3)<0, the curve is concave down, confirming a local maximum. Substituting x=3 back into g(x):
g(3)=2ln(3−2)−(3)2+4(3)+1
g(3)=2ln(1)−9+12+1=0+4=4
The local maximum value of the function is 4.